Hajer Bahouri
Tunis University
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Featured researches published by Hajer Bahouri.
American Journal of Mathematics | 1999
Hajer Bahouri; Patrick Gérard
This work is devoted to the description of bounded energy sequences of solutions to the equation (1) □u + |u|4 = 0 in [inline-graphic xmlns:xlink=http://www.w3.org/1999/xlink xlink:href=01i /], up to remainder terms small in energy norm and in every Strichartz norm. The proof relies on scattering theory for (1) and on a structure theorem for bounded energy sequences of solutions to the linear wave equation. In particular, we infer the existence of an a priori estimate of Strichartz norms of solutions to (1) in terms of their energy.
Annales De L Institut Henri Poincare-analyse Non Lineaire | 1998
Hajer Bahouri; Jalal Shatah
Abstract In this paper we prove that finite energy solutions (with added regularity) to the critical wave equation □u + u5 = 0 on R 3 decay to zero in time. The proof is based on a global space-time estimate and dilation identity.
Journal D Analyse Mathematique | 2000
Hajer Bahouri; Patrick Gérard; Chao-Jiang Xu
In this paper, we prove dispersive and Strichartz inequalities on the Heisenberg group. The proof involves the analysis of Besov-type spaces on the Heisenberg group.
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin
In Chapter 2 we give a detailed presentation on Littlewood-Paley decomposition and define homogeneous and nonhomogeneous Besov spaces. We should emphasize that we have replaced the usual definition of homogeneous spaces (which are quotient distribution spaces modulo polynomials) by something better adapted to the study of partial differential equations (indeed, dealing with distributions modulo polynomials is not appropriate in this context). We also establish technical results (commutator estimates and functional inequalities, in particular) which will be used in the following chapters.
Archive | 1997
Hajer Bahouri; Patrick Gérard
This paper is devoted to generalized geometrical optics for the following nonlinear wave equation with critical exponent, n n
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin
square u + left| u right|^4 u = 0
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin
n n(1) n nwhere (square = partial _t^2 - Delta _x ,t in {text{R,}},x in {text{R}}^{text{3}} ). The global well-posedness of equation (1) in the energy space was proved rather recently by Shatah-Struwe [16]. Let us recall precisely this result: given (phi in dot H^1 left( {{text{R}}^{text{3}} } right),psi in L^2 left( {{text{R}}^{text{3}} } right)) there exists a unique solution u to (1) satisfying (uleft| {_{t = 0} = phi ,,partial _t u} right.left| {_{t = 0} = psi } right.)and (u in L_{{text{loc}}}^5 left( {{text{R}},L^{10} left( {{text{R}}^{text{3}} } right)} right)). Observe that this latter property means exactly that the nonlinear term (left| u right|^4 u) in (1) belongs to (L_{{text{loc}}}^1 left( {{text{R,}},L^2 left( {{text{R}}^{text{3}} } right)} right)), which allows us to consider it as a source term in the energy method. In particular, this implies (left( {u,partial _t u} right) in Cleft( {{text{R}}_t ,dot H^1 left( {{text{R}}^{text{3}} } right) times L^2 left( {{text{R}}^{text{3}} } right)} right)) with conservation of energy n n
Archive | 2011
Hajer Bahouri; Jean-Yves Chemin; Raphaël Danchin